The Morphology of Complex Materials: MTEN 657 MWF 3:00-3:50 Baldwin 641 Prof. Greg Beaucage
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Transcript of The Morphology of Complex Materials: MTEN 657 MWF 3:00-3:50 Baldwin 641 Prof. Greg Beaucage
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The Morphology of Complex Materials: MTEN 657
MWF 3:00-3:50 Baldwin 641Prof. Greg Beaucage
β-Sheetwebhost.bridgew.edu/fgorga/proteins/beta.htm
Aggregated Nanoparticlesfrom Lead Based Paint
“Emerging Issues in Nanoparticle Aerosol Science and Technology (NAST)”
NSF 2003
Course Requirements:
-Weekly Quiz (8 to 9 in quarter)-Comprehensive Final (worth 3
quizzes)
-Old Quizzes will serve as homework
(These have posted answers)I may also assign other homework
where it is needed
You can replace quiz grades with a (or several) report(s) on a topical
area not covered in class but pertaining to the hierarchy of
morphology for a complex material. Several examples are given on the
web page.
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Structural Hierarchy of Complex Materials
Consider that we would like to understand a forest, such as the Amazon Forestfrom a Structural Perspective in order to develop predictive capabilities and an understanding
of the basic features to such a complex structure.
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Structural Hierarchy of Complex Materials
Consider that we would like to understand a forest, such as the Amazon Forestfrom a Structural Perspective in order to develop predictive capabilities and an understanding
of the basic features to such a complex structure.
http://www.eng.uc.edu/~gbeaucag/Classes/MorphologyofComplexMaterials/Overview.html
1) The first logical step is to consider a base (primary) unit for the forest and
2) then devise a repetition or branching rule (fractal scaling law) to create trees (secondary structure).
We revise the scaling rules and primary unit until we produce the type of trees we are interested in.
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Structural Hierarchy of Complex Materials
Consider that we would like to understand a forest, such as the Amazon Forestfrom a Structural Perspective in order to develop predictive capabilities and an understanding
of the basic features to such a complex structure.
http://www.eng.uc.edu/~gbeaucag/Classes/MorphologyofComplexMaterials/Overview.html
We could consider other types of trees in the same way.
3) Trees form clusters or groves (tertiary structure) that can follow a spacing and shape rule, for instance, redwoods grow in “fairy” rings or “cathedral” groups
around an old tree.
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Structural Hierarchy of Complex Materials
Consider that we would like to understand a forest, such as the Amazon Forestfrom a Structural Perspective in order to develop predictive capabilities and an understanding
of the basic features to such a complex structure.
4) Groupings of groves of trees interact with the environment to form forests (quaternary structures)
5) Higher levels of organization can be considered
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Structural Hierarchy of Complex Materials
-We have considered discrete “levels” of structure within a hierarchical model.
-In constructing the hierarchy is it natural to start from the smallest scale and to build up.
-We have borrowed from proteins in labeling the hierarchical levels primary, secondary, tertiary and quaternary.
-The hierarchical approach gives insight into how complex natural systems can be understood as if the structural levels acted independently in some respects.
-One of the main insights from hierarchical models is to understand in detail how and why structural levels are not independent and how they can interact to
accommodate the environment.
-In this course we will consider the application of hierarchical models to understand complex molecular systems with the goal of understanding how the hierarchical
approach can be expanded.
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Topics we will cover:
1) Protein structure (the origin of the hierarchical concept) 3 weeks
2) DNA and RNA structure (first adaptation of the hierarchical approach)1 week
3) Polymer Chain Structure in Solution (a statistical hierarchy) 2 weeks
4) Hierarchy of Polymer Dynamics in Solution (a kinetic hierarchy) 1 week
5) Polymer Crystalline Structure (hierarchy in a structural material) 2 weeks
6) Branched Fractal Aggregates (hierarchy in a statistical structural material)1 week
Structural Hierarchy of Complex Materials
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Twig
Tree/Branching
Grove/Cluster
Structural Hierarchy of Complex Materials
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The StructuralHierarchy of Proteins
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Size of proteins.html
Four Levels of Protein Structure.html
http://learn.genetics.utah.edu/content/begin/cells/scale/
http://www.youtube.com/watch?v=y8Z48RoRxHg&feature=related
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http://www.friedli.com/herbs/phytochem/proteins.html#peptide_bond
The α-carbon is a chiral centerit is always in an L-configuration spelling “CORN” in the Newman projection
There are 20 choices for the “R” group in nature. This makes an alphabet from which sequences of these 20 letters can code for any protein. Depending on the chemical functionality of the “R” groups different properties, polarity, hydrophobicity, ability to bond by disulfide linkages, hydrogen bonding and chain flexibility or rigidity can be imparted to the protein.
Quick Look at Amino Acids.htmlhttp://www.johnkyrk.com/aminoacid.html
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Amino Acids.html
3D Amino Acids
http://www.bioscience.org/urllists/aminacid.htm
http://www.mcb.ucdavis.edu/courses/bis102/Polar.html
More Amino Acidshttp://biology.clc.uc.edu/courses/bio104/protein.htm
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Methionine Start Amino Acid (usually removed in later steps)
Glycine -H Flexible non-polarAlanine -CH3 Flexible non-polar
Proline 10-40% Cis Configuration depending on neighboring amino acid residues Found in Turns and at start of α-helix
Cystine Disulfide Linkages (Hair is 5% cystine)
Hydrogen Bonding in Kevlar
NH = DonorC=O = Acceptor
Polyamides are similar to proteins
Know These 5 Amino Acids Well
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The Genetic Code Links.html
Post Translational Modification
of Insulin
Movie of Protein Synthesishttp://nutrition.jbpub.com/resources/animations.cfm?id=14&debug=0
http://www.eng.uc.edu/~gbeaucag/Classes/MorphologyofComplexMaterials/GeneticCode.html
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The Peptide Bond
Resonance structures make the peptide group planar (like a card).
Proline is the exception Proline adds main chain curvature
found in turns and at start of α-helix
http://www.friedli.com/herbs/phytochem/proteins.html#peptide_bond
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The peptide linkage forms a planar structure with the two α-carbons and the N,
H, C and O atoms
PSI ψ is the rotation angle between the carboxyl C and the α-carbon
PHI Φ is the rotation angle between N and the α-carbon
Certain values of these two rotation angles are preferred in certain structures
So the angles serve as a map for the protein secondary structure
http://www.friedli.com/herbs/phytochem/proteins.html#peptide_bond
Fully Extended Chain (Planar Zig-Zag)Phi/Psi 180, 180
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olunderstandconfo.html
http://visu.uwlax.edu/BioChem/Rotate.mov Phi rotation for Psi = 0
Psi rotation for Phi = 0
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olunderstandconfo.html
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Folding Simple Dynamic Simulation.html
More Complicated Simulation.html
Yet more complicated.html
Where and When do Proteins Fold.html
Small Protein Folding.html
Another Small Protein Folding.html
Folding a Protein by Hand.html
Entropy and Protein Folding.html
Folding of Villin.html
Lets Jump Ahead and Look at Protein Folding
http://intro.bio.umb.edu/111-112/111F98Lect/folding.html
http://www.youtube.com/watch?v=_xF96sNWnK4&feature=related
http://www.cs.ucl.ac.uk/staff/D.Jones/t42morph.html
http://www.youtube.com/watch?v=meNEUTn9Atg
http://www.youtube.com/watch?v=BrUdCVwgJxc&feature=related
http://www.youtube.com/watch?v=E0TX3yMEZ8Y&feature=related
http://www.youtube.com/watch?v=va92d9Ei1QM&feature=related
http://www.youtube.com/watch?v=gaaiepNVyvE&feature=related
http://www.youtube.com/watch?v=1eSwDKZQpok&feature=related
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Secondary Structures of Proteinsα-Helix, β-Sheets, Turns
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pdb of α-Helixhttp://employees.csbsju.edu/hjakubowski/Jmol/alpha_helix/alpha_helix.htm
Right Handed α-Helix
http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olunderstandconfo.html
C=O from residue “i”hydrogen bonds with
NH from residue “i+4”
Phi/Psi angles are -57, -47
Residues per turn = 3.6Rise per turn = 5.4 Å
Amino Acids and HelixGlycine too flexible
Proline too rigidShort H-Bonding (Ser, Asp, Asn) Disrupt Coil
Long H-Bonding are OKBranches at α-C Disrupt Coil (Val, Ile)
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olunderstandconfo.html
Valine
Isoleucine
Serine
Asparagine
AsparticAcid
Glycine
Proline
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Other Types of Helices
310 helix
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β-Sheets
Phi PsiParallel -119 +113Anti-Parallel -139 +135α-Helix -57 -47Extended ±180 ±180
Rippled Sheets
H-Bonding between strands in SheetH-Bonding within strand in Helix
Parallel => 12 member ringsAnti-Parallel => 14 and 10 member rings alternating
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Parallel β-Sheets
12-member rings
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Anti-Parallel β-Sheets
Alternating 10- and 14-member rings
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Twisted β-Sheet/Saddle
Twisted β-Saddle
http://employees.csbsju.edu/hjakubowski/Jmol/Twisted%20Beta%20Sheet/Twisted_Beta_Sheet.htm
β-Barrel
β-Barrelhttp://employees.csbsju.edu/hjakubowski/Jmol/beta_barrel_tpi/Beta_Barrel_tpi.htm
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olunderstandconfo.html
Valine
Isoleucine
Serine
Asparagine
AsparticAcid
Glycine
Proline
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β-Turns
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β-Turns
Reverse Turnhttp://employees.csbsju.edu/hjakubowski/Jmol/RevTurnTryInhib/revturnTrpInhib.htm
Type 2 and Type 1 Reverse Turns
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Micelles (Vesicle)
Dodecylphosphocholine (DPC) Micelle
http://employees.csbsju.edu/hjakubowski/Jmol/Micelle/micelle.htm
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Protein with a buried hydrophobic grouphttp://employees.csbsju.edu/hjakubowski/Jmol/HAAPBJmol/HAAPBBovineBuryF10.htm
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~50% of amino acids are in well defined secondary structures27% in α-helix and 23% in β-sheets
Native state proteins have a packing density slightly higher than FCC/HCP 0.75 vs 0.74
Organic liquids 0.6-0.7 Synthetic Polymer Chain in Solution ~0.001 So the transition from an unfolded protein in solution to a native state protein
involves a densification of about 750 to 1000 times.
Nonpolar 83% internal, Charged 54% exposed, uncharged 63% internal
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Super-Secondary Structures
Common motifs
Helix-Loop-Helix
EF-Hand
http://employees.csbsju.edu/hjakubowski/Jmol/Lambda_Repressor/Lambda_Repressor.htm
http://employees.csbsju.edu/hjakubowski/Jmol/Calmodulin_EF_Hand/Calmodulin_EF_Hand.htm
DNA and Calcium Binding sites
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β-Hairpin or Beta-Beta in Anti-Parallel Structures
Super-Secondary Structures
http://employees.csbsju.edu/hjakubowski/Jmol/Bovine%20Pancreatic%20Trypsin%20Inhibitor/Bovine_Pancreatic_Trypsin_Inhibitor.htm
Greek Key Motif
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Beta-Alpha-Beta (to connect two parallel β-sheets)http://employees.csbsju.edu/hjakubowski/Jmol/BETA-ALPHA-BETA_MOTIFF/BETA-ALPHA-BETA_MOTIFF.htm
β-Helicieshttp://cti.itc.virginia.edu/~cmg/Demo/pdb/ap/ap.htm
(seen in pathogens, viruses, bacteria)
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Many β-Topologies
http://www.cryst.bbk.ac.uk/PPS2/course/section10/all_beta.html
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3 Classes of Proteins (Characteristic Secondary Structures)
α-Proteins
αβ-Proteins
β-Proteins
Cytochrome B562http://employees.csbsju.edu/hjakubowski/Jmol/Cytochrome_B562/Cytochrome_B562.htm
Met-Myoglobinhttp://employees.csbsju.edu/hjakubowski/Jmol/Met-Myoglobin
Triose Phosphate Isomerasehttp://employees.csbsju.edu/hjakubowski/Jmol/Triose%20Phosphate%20Isomerase/TRIOSE_PHOSPHATE_ISOMERASE.htm
Hexokinasehttp://employees.csbsju.edu/hjakubowski/Jmol/Hexokinase/HEXOKINASE.htm
Superoxide Dismutasehttp://employees.csbsju.edu/hjakubowski/Jmol/Superoxide%20Dismutase/SUPEROXIDE_DISMUTASE.htm
Human IgG1 Antibodyhttp://employees.csbsju.edu/hjakubowski/Jmol/Human%20Antibody%20Molecule-IgG1/Human_Antibody_Molecule%C2%AD_IgG1.htm
Retinol Binding Proteinhttp://employees.csbsju.edu/hjakubowski/Jmol/Retinol%20Binding%20Protein/RETINOL_BINDING_PROTEIN.htm
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Fibrillar (elastic) versus Globular Proteins
Elastin (Blood Vessels) β-sheets and α-helicies with β-turns
Reslin (Insects Wings)
Silk (Spiders etc.) β-sheets and α-helicies with β-turns
Fibrillin (Cartilage) - Folded β-Sheet like and Accordian
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Tertiary Structure and Protein Folding
Consider a protein of 100 residues each with two bond angles Φ and ψ that can take 3 positions each so 9 conformations. The
chain has 9100 = 2.7 x 1095 conformations. Even with 10-13s to change a conformation, it
would take 8.4 x 1074 years to probe all conformations (that is along time).
Such a protein folds in less than a second. This is called Levinthal’s Paradox.
The key to resolving Levinthal’s Paradox is to limit the choices.
Disulfide bonds are a major limiting factor,Consider Ribonuclease (RNase A) (an enzyme that degrades RNA)
Having 4 disulfide bonds that serve as tethers for the folding process.
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Folds “like a taco” to bind with the RNA substrate
Armour purified 1 kilo and gave it away for study
124 residues 13.7 kDaPolycation that binds with polyanionic RNA
Positive charges are in the taco cleft.
RNase Ahttp://www.rcsb.org/pdb/explore/jmol.do?structureId=7RSA&bionumber=1
Nobel Prize Lecture published as:Anfinsen, C.B. (1973) "Principles that govern the folding of protein chains." Science
181 223-230.
Anfinsen Postulate: For Small Globular Proteins the Tertiary Structure is determined only by the
amino acid sequence
http://employees.csbsju.edu/hjakubowski/Jmol/RNase/RNase.htm
RNase Structure
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β-Mercapto Ethanol
Urea
Competes with H-BondsDenatures (Destablizes) Proteins
Competes with H-BondsDenatures (Destablizes) Proteins
Guanidine-HCl
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olprotfold.html
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http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olprotfold.html
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Native state is a “Global Minimum in Free Energy”Folding Process Occurs on an Energy “Funnel”
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Folding does not occur by a single pathway, but is a statistical processof searching the energy landscape for minima
For large proteins we see intermediates, molten globules, non-biologically active dense states
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Simple proteins undergo a cooperative process
y-axis could be viscosity (hydrodynamic radius),
circular dichroism, fluorescence,
diffusion coefficient (hydrodynamic radius) from dynamic light scattering,
radius of gyration from static light scattering
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Viscosity
Native state has the smallest volume
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Mass Fractal Dimension, 1 ≤ df ≤ 3
Mass ~ Size1
Mass ~ Size2
1-d df = 1
df = 22-d
Mass ~ Size3 df = 33-d
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Mass Fractal Dimension, 1 ≤ df ≤ 3
Mass ~ Size2
Mass ~ Size1.67
2-d df = 2
df = 5/3
Random (Brownian) Walkθ-Solvent Condition
Self-Avoiding Walk/Expanded CoilGood Solvent Condition
In the collapse transition from an expanded coil to a native state for a protein of 100 residues (N = Mass = 100)
Size ~ 15.8 for Expanded Coil (10 for Gaussian) and 4.6 for Native State
For N = 10000 this becomes 251 : 100 : 21.5For large proteins the change in size is dramatic (order of
10x)
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Viscosity
For the Native State Mass ~ ρ VMolecule
Einstein Equation (for Suspension of 3d Objects)
For “Gaussian” Chain Mass ~ Size2 ~ V2/3
V ~ Mass3/2
For “Expanded Coil” Mass ~ Size5/3 ~ V5/9
V ~ Mass9/5
For “Fractal” Mass ~ Sizedf ~ Vdf/3
V ~ Mass3/df
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Viscosity
For the Native State Mass ~ ρ VMolecule
Einstein Equation (for Suspension of 3d Objects)
For “Gaussian” Chain Mass ~ Size2 ~ V2/3
V ~ Mass3/2
For “Expanded Coil” Mass ~ Size5/3 ~ V5/9
V ~ Mass9/5
For “Fractal” Mass ~ Sizedf ~ Vdf/3
V ~ Mass3/df
“Size” is the“Hydrodynamic Size”
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Circular Dichroism
Light Polarizationhttp://www.enzim.hu/~szia/cddemo/edemo0.htm?CFID=1025184&CFTOKEN=88815524
CD Spectroscopy for Proteins
http://www.cryst.bbk.ac.uk/PPS2/course/section8/ss-960531_21.html
Wikipedia on CDhttp://en.wikipedia.org/wiki/Circular_dichroism
http://www.ruppweb.org/cd/cdtutorial.htm
Difference in Absorption
Molar Circular Dichroism (c = molar concentration)
Degrees of Ellipticity
These change with the extent and nature of secondary structure such as helicies
Examples of CDhttp://www.ap-lab.com/circular_dichroism.htm
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Static Light Scattering for Radius of Gyration
Guinier’s Law
Beaucage G J. Appl. Cryst. 28 717-728 (1995).
€
γGaussian r( ) = exp −3r2
2σ 2( )
σ 2 =
xi −μ( )2
i=1
N
∑N −1
= 2Rg2
€
I q( ) = IeNne2 exp
−Rg2q2
3 ⎛
⎝ ⎜
⎞
⎠ ⎟
Lead Term is
€
I(1/ r) ~ N r( )n r( )2
€
I(0) = Nne2
€
γ0 r( ) =1−S
4Vr +...
A particle with no surface
€
r⇒ 0 then d γGaussian r( )( )
dr⇒ 0
Consider binary interference at a distance “r” for a particle with arbitrary orientationRotate and translate a particle so that two points separated by r lie in the particle for all rotations
and average the structures at these different orientations
Binary AutocorrelationFunction
Scattered Intensity is the Fourier Transform ofThe Binary Autocorrelation Function
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For qRg >> 1
df = 2
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For static scattering p(r) is the binary spatial auto-correlation function
We can also consider correlations in time, binary temporal correlation functiong1(q,τ)
For dynamics we consider a single value of q or r and watch how the intensity changes with timeI(q,t)
We consider correlation between intensities separated by tWe need to subtract the constant intensity due to scattering at different size scales
and consider only the fluctuations at a given size scale, r or 2π/r = q
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Dynamic Light Scattering
a = RH = Hydrodynamic Radius
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Dynamic Light Scattering
http://www.eng.uc.edu/~gbeaucag/Classes/Physics/DLS.pdf
my DLS web page
Wikihttp://webcache.googleusercontent.com/search?q=cache:eY3xhiX117IJ:en.wikipedia.org/wiki/Dynamic_light_scattering+&cd=1&hl=en&ct=clnk&gl=us
Wiki Einstein Stokes
http://webcache.googleusercontent.com/search?q=cache:yZDPRbqZ1BIJ:en.wikipedia.org/wiki/Einstein_relation_(kinetic_theory)+&cd=1&hl=en&ct=clnk&gl=us
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Optical Tweezers
Dielectric particles are attracted to the center of a focused beamScattering Force moves particles downstream
Force can be controlled with intensity of laser
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Stretching of a single protein (RNase)
http://employees.csbsju.edu/hjakubowski/classes/ch331/protstructure/olprotfold.html
Blue: Stretch just DNA linker moleculesRed: Stretch DNA and ProteinGreen: Release tension on Protein/DNA
Link to Paper at Sciencehttp://www.sciencemag.org/content/309/5743/2057
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It's been estimated that over half of all native proteins have regions (greater than 30
amino acids) that are disordered, and upwards of 20% of proteins are completely
disordered.
Natively Unfolded Proteins
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Membrane Proteins
http://blanco.biomol.uci.edu/mp_assembly.html
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http://blanco.biomol.uci.edu/translocon_machinery.html
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http://www.portfolio.mvm.ed.ac.uk/studentwebs/session2/group5/introliz.htm
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Electron transport chain is part of the ATP/ADP energy generation pathway for cellsThis involves many tertiary protein structures. For instance, Complex III is a quaternary structureof 9 proteins.
Heme B group
Quaternary Structures
http://en.wikipedia.org/wiki/Electron_transport_chain
http://proteopedia.org/wiki/index.php/Complex_III_of_Electron_Transport_Chain
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Quaternary Structure Page
http://proteopedia.org/wiki/index.php/Main_Page
Ribosome
http://proteopedia.org/wiki/index.php/Ribosome
Poly(A) Polymerase
http://proteopedia.org/wiki/index.php/2q66
Ribosome in Actionhttp://www.youtube.com/watch?v=Jml8CFBWcDs
Role of Ribosome
http://www.cytochemistry.net/cell-biology/ribosome.htm
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DNA/Protein Quaternary Structureshttp://www.biochem.ucl.ac.uk/bsm/prot_dna/prot_dna_cover.html
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RNA structure
Ribose
http://www.rnabase.org/primer/
t-RNA (Folded Structure)Deoxyribose
DNA
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If it takes DNA/RNA to template a protein and proteins to make/control DNA/RNAWhich came first Proteins or Nucleic Acids?
RNA World Hypothesis:
http://en.wikipedia.org/wiki/RNA_world_hypothesis
http://exploringorigins.org/rna.html
L1 Ligase Ribozyme
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Hierarchy of a Chromosome
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Core Histone
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http://www.eng.uc.edu/~gbeaucag/Classes/MorphologyofComplexMaterials/Physics%20of%20Chromatin%20Schiessel%202003.pdf
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